Method and apparatus for controlling resonant frequency of an optical interferometer cavity

• US 4,293,223 A
• Filed: 09/27/1979
• Issued: 10/06/1981
• Est. Priority Date: 09/27/1979
• Status: Expired due to Term

• Current Assignee: Norman T. Seaton
• Original Assignee: Norman T. Seaton
• Inventors: Seaton, Norman T.
• Primary Examiner(s): Clark, Conrad J.
• Assistant Examiner(s): Koren, Matthew W.
• Application Number:
  US06/079,324
• Time in Patent Office: 740 Days
• Field of Search: 356/352, 331/94.5 C
• US Class Current: 356/480
• CPC Class Codes: H01S 3/105 by controlling the mutual position or the reflecting properties of the reflectors of the cavity , e.g. by controlling the cavity lengthH01S3/10076, H01S3/13 take precedence

Abstract

An apparatus and method for controlling the resonant frequency of an optical interferometer cavity having a part having a dimension defining the resonant frequency. An electrical conductor adapted for connection to a source of electrical potential is mounted on and mechanically secured to the part of the cavity which has the dimension defining the resonant frequency. The electrical conductor provides a conduction path substantially parallel to the frequency defining dimension of the aforementioned cavity part and has a coefficient of thermal expansion. Mechanical force is transmitted to the aforementioned cavity part as a function of electrothermally induced change in the length of the electrical conductor, thus causing a change in the resonant frequency of the cavity.

Claims

1. A frequency control apparatus for an optical interferometer cavity having a part having a dimension defining resonant frequency comprising:

a plurality of substantially straight electrical conductors adapted for connection to a source of electrical potential and mounted on and mechanically secured to said part and providing a conduction path substantially parallel to said dimension and having a coefficient of thermal expansion and functioning to transmit mechanical force to said part as a function of electro-thermally induced change in length of said conductors for changing said resonant frequency.

2. The structure of claim 1 wherein said optical interferometer cavity comprises a laser tube having a wall providing said part;

and

said conduction path is substantially parallel to the longitudinal axis of said tube.

3. The structure of claim 2, said electrical conductors mounted on said wall substantially parallel to said axis with said conductors mounted in substantially uniformly circumferentially spaced relation on said wall.

4. The structure of claim 2, said electrical conductors connected in series and mounted on said wall substantially parallel to said axis with said conductors mounted in substantially uniformly circumferentially spaced relation on said wall.

5. The structure of claim 2, said electrical conductors connected in parallel and mounted in substantially uniformly circumferentially spaced relation on said wall.

6. The structure of claim 2, said electrical conductors connected in series-parallel and mounted in substantially uniformly circumferentially spaced relation on said wall.

7. The structure of claim 3 and an electrically conductive surface relieved to define said conductors and mounted on and bonded to said wall.

8. The structure of claim 3, said conductors being substantially continuously bonded over their length to said wall.

9. The structure of claim 2 and a sleeve mounted in encircling engagement on said wall;

and

said conductors comprising a wire wound lengthwise on and distributed evenly around and bonded to said sleeve with at least one of said wire and sleeve bonded to said wall.

10. A method of controlling the resonant frequency of an optical interferometer cavity having a part having a dimension defining resonant frequency comprising:

a. mechanically securing to said part a plurality of substantially straight electrical conductors having a coefficient of thermal expansion and having a conduction path substantially parallel to said dimension and having means for connection to a source of electrical potential;

b. generating a mechanical force by connecting said conductors to a source of electrical potential thus causing an electro-thermally induced change in length of said conductors; and

c. transmitting said mechanical force to said part thus changing said dimension.

11. The method of claim 11 wherein said optical interferometer cavity comprises a laser tube having a wall providing said part with said electrical conductors mounted on said wall substantially parallel to the longitudinal axis of said tube and in substantially uniformly circumferentially spaced relation on said wall said conductors being substantially continuously bonded over their length to said wall for transmitting their change-in-length force to said wall.